%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
%                                                                    %
%                Neutrinos and Supersymmetry                         %
%                                                                    %
%                file=book01macros.tex                               %
%                                                                    %
%               Last changed 20/3/2003 by JCR                        %
%                                                                    %
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%

%% From the approximate paper
\newcommand{\Sol}  {\mathsc{sol}}
\newcommand{\Dms}  {\Delta m^2_\Sol}
\DeclareMathAlphabet{\mathsc}{OT1}{cmr}{m}{sc}


%%  From Neutralino decays paper
\newcommand {\sect} [1] {Sec.~\ref{#1}}
\newcommand {\app} [1] {Appendix~\ref{#1} }
\def\eq#1{{eq. (\ref{#1})}}
\def\Eq#1{{Eq.~(\ref{#1})}}
\newcommand {\chiz} [1] {\tilde{\chi}^{0}_{#1} }
\newcommand {\no} {\nonumber \\}
\newcommand {\sina} {\sin \alpha}
\newcommand {\cosa} {\cos \alpha}
\newcommand {\cosaq} {\cos^2 \alpha}
\newcommand {\sinaq} {\sin^2 \alpha}
\newcommand {\mchiz} [1] {m_{\tilde{\chi}^{0}_{#1} }}
\newcommand {\figz} [2] {Fig.~(\ref{#1}{#2})}
\newcommand {\fig} [1] {Fig.~\ref{#1}}
\newcommand {\tab} [1] {Table~\ref{#1}}
%%

%% From Stau decays paper
\newcommand{\dof}{d.o.f.}
\def\te{{\tilde e}}
\def\tm{{\tilde \mu}}
\newcommand{\CL} {C.L.}
%%

\def\be{\begin{equation}}        
\def\ee{\end{equation}} 
\def\bear{\be\begin{array}}       
\def\eear{\end{array}\ee} 
\def\bea{\begin{eqnarray}} 
\def\eea{\end{eqnarray}} 
\def\SM{Standard Model } 
\def\baselinestretch{1.2} 
\def\vb#1{\vbox to #1 pt{}}
\def\beqa{\begin{eqnarray}}
\def\eeqa{\end{eqnarray}}
\def\ni{\noindent}
\def\nn{\nonumber}
\def\beq{\begin{equation}}
\def\eeq{\end{equation}}
\def\ba{\begin{array}}
\def\ea{\end{array}}
\def\ovl{\overline}
\def\ds{\displaystyle}
\def\np#1#2#3{           {\sl Nucl. Phys. }{\bf #1} (#2) #3}
\def\pl#1#2#3{           {\sl Phys. Lett. }{\bf #1} (#2) #3}
\def\pr#1#2#3{           {\sl Phys. Rev. }{\bf #1} (#2) #3}
\def\prep#1#2#3{         {\sl Phys. Rep. }{\bf #1} (#2) #3}
\def\prl#1#2#3{          {\sl Phys. Rev. Lett. }{\bf #1} (#2) #3}
\def\epj#1#2#3{          {\sl Eur. Phys. J. }{\bf #1} (#2) #3}
%======================================== 
\def\sqrthalf{{\textstyle{1 \over \sqrt{2}}}} 
\def\slash#1{#1\!\!\! /}
\def\Slash#1{#1\!\!\!\! /}

\def\21{$SU(2) \ot U(1)$} 
\def\ot{\otimes} 
\def\ie{{\it i.e.}} 
\def\etal{{\it et al.}} 
\def\half{{\textstyle{1 \over 2}}} 
\def\third{{\textstyle{1 \over 3}}} 
\def\quarter{{\textstyle{1 \over 4}}} 
\def\fourth{{\textstyle{1 \over 4}}} 
\def\sixth{{\textstyle{1 \over 6}}} 
\def\eighth{{\textstyle{1 \over 8}}} 
\def\bold#1{\setbox0=\hbox{$#1$} 
     \kern-.025em\copy0\kern-\wd0 
     \kern.05em\copy0\kern-\wd0 
     \kern-.025em\raise.0433em\box0 } 
\def\VCKM#1{{\bold{V}^{\hbox{\tiny CKM}}_{#1}}}
\def\smallfrac#1#2{{\textstyle{#1 \over #2}}}
\def\ms{\medskip}
\def\bs{\bigskip}
\def\cl{\centerline}
\def\ra{\rightarrow}
\def\vev#1{\left\langle #1\right\rangle}
\def\ket#1{\left\vert #1\right\rangle}
\def\bra#1{\left\langle #1\right\vert}
\def\lrvpartial{{\partial \! \! \! \! \vbox to 12pt{}^{\leftrightarrow}}}
\def\lt{<}
\def\gt{>}
\def\lag{{\cal L}}
\def\rp{$R_p \hspace{-1em}/\;\:$ }
\def\Fig#1{Fig.~(\ref{#1})}
%
\newcommand {\ignore}[1]{}
\newcommand{\ptmis}{{ {\rm p} \hspace{-0.53 em} \raisebox{-0.27 ex} {/}_T }}
%
\newcommand{\LT}        {\left}
\newcommand{\RT}        {\right}
\newcommand{\0}         {\hphantom{0}}
\renewcommand{\ne}      {\hbox{$\nu_e$} }
\newcommand{\nm}        {\hbox{$\nu_\mu$} }
\newcommand{\nt}        {\hbox{$\nu_\tau$} }
\def\ltap{\ \raisebox{-.4ex}{\rlap{$\sim$}} \raisebox{.4ex}{$<$}\ }
\def\gtap{\ \raisebox{-.4ex}{\rlap{$\sim$}} \raisebox{.4ex}{$>$}\ }
\newcommand{\pnu}[1] {\overset{\smash{\scriptscriptstyle (-)}}{\nu}_{\hskip-3pt #1}}
\def\lsim{\mathrel{\rlap{\lower4pt\hbox{\hskip1pt$\sim$}}
    \raise1pt\hbox{$<$}}}         %iless than or approx. symbol
\def\gsim{\mathrel{\rlap{\lower4pt\hbox{\hskip1pt$\sim$}}
    \raise1pt\hbox{$>$}}}         %greater than or approx. symbol
\def\baselinestretch{1.5}
\newcommand{\sm}{{Standard Model}}

%-- command (re)definitions -----------------------------------------

\newcommand{\capdef}{}
\newcommand{\mycaption}[2][\capdef]{\renewcommand{\capdef}{#2}%
        \caption[#1]{{\itshape #2}}} 
\makeatletter
\renewcommand{\fnum@table}{\textbf{\tablename~\thetable}}
\renewcommand{\fnum@figure}{\textbf{\figurename~\thefigure}}
\makeatother

%%%from pol%%%

%% upright Greek letters (example below: upright "mu")
\newcommand{\greeksym}[1]{{\usefont{U}{psy}{m}{n}#1}}
\newcommand{\umu}{\mbox{\greeksym{m}}}
\newcommand{\udelta}{\mbox{\greeksym{d}}}
\newcommand{\uDelta}{\mbox{\greeksym{D}}}
\newcommand{\uPi}{\mbox{\greeksym{P}}}
%%
\def\mxth{\mathsurround=0pt }
\def\xversim#1#2{\lower2.pt\vbox{\baselineskip0pt \lineskip-.5pt
  \ialign{$\mxth#1\hfil##\hfil$\crcr#2\crcr\sim\crcr}}}             
\def\gtrsim{\mathrel{\mathpalette\xversim >}}                                    
\def\lesssim{\mathrel{\mathpalette\xversim <}}    
%%
%%
\newcommand{\postscript}[2]
{\setlength{\epsfxsize}{#2\hsize}
\centerline{\epsfbox{#1}}}
%%
% Some other macros used in the sample text
\def\st{\scriptstyle}
\def\sst{\scriptscriptstyle}
\def\mco{\multicolumn}
\def\be{\begin{equation}}
\def\ee{\end{equation}}
\def\bea{\begin{eqnarray}}
\def\eea{\end{eqnarray}}
\def\CPbar{\hbox{{\rm CP}\hskip-1.80em{/}}}%temp replacemt due to no font
%%
\def\mweak{M_{\rm Weak}}
\def\mplanck{M_{\rm Planck}}
\def\hc{\it {h.c.}}
%%

%%%%%%%%%%%%%%%% spectrum notation:%%%%%%%%%%%%%%%

%mirror superfields
\newcommand{\mrU}{{U}^{\prime}}
\newcommand{\mrD}{{D}^{\prime}}
\newcommand{\mrQ}{{Q}^{\prime}}
\newcommand{\mrL}{{L}^{\prime}}
\newcommand{\mrE}{{E}^{\prime}}
\newcommand{\mrN}{{N}^{\prime}}
\newcommand{\mrQthird}{{{Q}^{\prime}}_3}
%sfermions
\newcommand{\sU}{{\widetilde{U}}}
\newcommand{\sD}{{\widetilde{D}}}
\newcommand{\sQ}{{\widetilde{Q}}}
\newcommand{\sL}{{\widetilde{L}}}
\newcommand{\sE}{{\widetilde{E}}}
\newcommand{\sN}{{\widetilde{N}}}
\newcommand{\sQthird}{{\widetilde{Q}_3}}
%mirror sfermions
\newcommand{\mrsU}{{\widetilde{U^{\prime}}}}
\newcommand{\mrsD}{{\widetilde{D^{\prime}}}}
\newcommand{\mrsQ}{{\widetilde{Q^{\prime}}}}
\newcommand{\mrsL}{{\widetilde{L^{\prime}}}}
\newcommand{\mrsE}{{\widetilde{E^{\prime}}}}
\newcommand{\mrsN}{{\widetilde{N^{\prime}}}}
\newcommand{\mrsQthird}{{{\widetilde{Q^{\prime}}}}_3}
%mirror quarks
\newcommand{\mru}{{u}^{\prime}}
\newcommand{\mruL}{{u}^{\prime}_{L}}
\newcommand{\mruR}{{u}^{\prime}_{R}}
\newcommand{\mrd}{{d}^{\prime}}
\newcommand{\mrdL}{{d}^{\prime}_{L}}
\newcommand{\mrdR}{{d}^{\prime}_{R}}
\newcommand{\mrq}{{q}^{\prime}}
%mirror 3rd family quarks 
\newcommand{\mrt}{{t}^{\prime}}
\newcommand{\mrtL}{{t}^{\prime}_{L}}
\newcommand{\mrtR}{{t}^{\prime}_{R}}
\newcommand{\mrb}{{b}^{\prime}}
\newcommand{\mrbL}{{b}^{\prime}_{L}}
\newcommand{\mrbR}{{b}^{\prime}_{R}}
%mirror 2nd family quarks 
\newcommand{\mrc}{{c}^{\prime}}
\newcommand{\mrcL}{{c}^{\prime}_{L}}
\newcommand{\mrcR}{{c}^{\prime}_{R}}
\newcommand{\mrs}{{s}^{\prime}}
\newcommand{\mrsl}{{s}^{\prime}_{L}}
\newcommand{\mrsR}{{s}^{\prime}_{R}}
%mirror leptons
\newcommand{\mrl}{{l}^{\prime}}
\newcommand{\mre}{{e}^{\prime}}
\newcommand{\mreL}{{e}^{\prime}_{L}}
\newcommand{\mreR}{{e}^{\prime}_{R}}
\newcommand{\mrtau}{{\tau}^{\prime}}
\newcommand{\mrtauL}{{\tau}^{\prime}_{L}}
\newcommand{\mrtauR}{{\tau}^{\prime}_{R}}
\newcommand{\mrmu}{{\mu}^{\prime}}
\newcommand{\mrmuL}{{\mu}^{\prime}_{L}}
\newcommand{\mrmuR}{{\mu}^{\prime}_{R}}
\newcommand{\mrnu}{{\nu}^{\prime}}
\newcommand{\mrnuL}{{\nuL}^{\prime}_{L}}
\newcommand{\mrnuR}{{\nuR}^{\prime}_{R}}
%Higgsses and mirror Higgses
\newcommand{\hu}{{H}_{2}}
\newcommand{\hd}{{H}_{1}}
\newcommand{\mrhu}{{H}^{\prime}_{2}}
\newcommand{\mrhd}{{H}^{\prime}_{1}}
%Higgsionos
\newcommand{\hinou}{{\widetilde{H}}_{2}}
\newcommand{\hinod}{{\widetilde{H}}_{1}}
%mirror Higgsionos
\newcommand{\mrhinou}{{\widetilde{H}}^{\prime}_{2}}
\newcommand{\mrhinod}{{\widetilde{H}}^{\prime}_{1}}
%gauginos
\newcommand{\bino}{\widetilde{B}}
\newcommand{\wino}{\widetilde{W}}
\newcommand{\gluino}{\widetilde{g}}
%adjoint
\newcommand{\adjoint}{\Phi_{V}}
\newcommand{\sadjoint}{\phi_{V}}
\newcommand{\fadjoint}{\psi_{V}}


\newcommand{\gadjoint}{\Phi_{g}}
\newcommand{\gsadjoint}{\phi_{g}}
\newcommand{\gfadjoint}{\psi_{g}}

\newcommand{\wadjoint}{\Phi_{W}}
\newcommand{\wsadjoint}{\phi_{W}}
\newcommand{\wfadjoint}{\psi_{W}}

\newcommand{\badjoint}{\Phi_{B}}
\newcommand{\bsadjoint}{\phi_{B}}
\newcommand{\bfadjoint}{\psi_{B}}

%other
\newcommand{\sNu}{{\widetilde{\nu}}}
\newcommand{\stau}{{\widetilde{\tau}}}
\newcommand{\smu}{{\widetilde{\mu}}}
\newcommand{\stt}{{\widetilde{t}}}
\newcommand{\sbb}{{\widetilde{b}}}
\newcommand{\scc}{{\widetilde{c}}}
\newcommand{\sss}{{\widetilde{s}}}
\newcommand{\mrsNu}{{\widetilde{\nu}}^{\prime}}
\newcommand{\mrstau}{{\widetilde{\tau}}^{\prime}}
\newcommand{\mrsmu}{{\widetilde{\mu}}^{\prime}}
\newcommand{\mrst}{{\widetilde{t}}^{\prime}}
\newcommand{\mrsb}{{\widetilde{b}}^{\prime}}
\newcommand{\mrsc}{{\widetilde{c}}^{\prime}}
\newcommand{\mrss}{{\widetilde{s}}^{\prime}}

%%%%end of pol%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%







